Topological insulator structure

ABSTRACT

A topological insulator structure includes an insulating substrate and a magnetically doped TI quantum well film located on the insulating substrate. A material of the magnetically doped TI quantum well film is represented by a chemical formula of Cr y (Bi x Sb 1-x ) 2-y Te 3 . 0&lt;x&lt;1, 0&lt;y&lt;2. Values of x and y satisfies that an amount of a hole type charge carriers introduced by a doping with Cr is substantially equal to an amount of an electron type charge carriers introduced by a doping with Bi. The magnetically doped TI quantum well film is in 3 QL to 5 QL.

RELATED APPLICATIONS

This application claims all benefits accruing under 35 U.S.C. §119 from China Patent Application No. 201210559564.X, filed on Dec. 21, 2012 in the China Intellectual Property Office, the disclosure of which is incorporated herein by reference. This application is related to commonly-assigned applications entitled, “METHOD FOR GENERATING QUANTIZED ANOMALOUS HALL EFFECT,” filed **** (Atty. Docket No. US50945); “ELECTRICAL DEVICE,” filed **** (Atty. Docket No. US50947); “METHOD FOR MAKING TOPOLOGICAL INSULATOR STRUCTURE,” filed **** (Atty. Docket No. US50948); and “TOPOLOGICAL INSULATOR STRUCTURE,” filed **** (Atty. Docket No. US50946).

BACKGROUND

1. Technical Field

The present disclosure relates to a topological insulator structure.

2. Discussion of Related Art

If an electric current flows through an electrical conductor in a magnetic field perpendicular to the electric current, a measurable voltage difference between two sides of the electrical conductor, transverses to the electric current and the magnetic field, will be produced. The presence of this measurable voltage difference is called the Hall effect (HE) discovered by E. H. Hall in 1879. Subsequently, the anomalous Hall effect (AHE) in magnetic materials and the spin Hall effect (SHE) in semiconductors were discovered. Theoretically, HE, AHE, and SHE would have corresponding quantized forms. In 1980, K. V. Klitzing et al. achieved quantum Hall effect (QHE) in a semiconductor in a strong magnetic field at a low temperature (Klitzing K. V. et al., New Method for High-Accuracy Determination of the Fine-Structure Constant Based on Quantized Hall Resistance, Phys Rev Lett, 1980, 45:494-497). After that, D. C. Tsui et al. achieved fractional quantum Hall effect (FQHE) during the studying of the HE in a stronger magnetic field (Tsui D. C. et al., Two-Dimensional Magnetotransport in the Extreme Quantum Limit. Phys Rev Lett, 1982, 48:1559-1562). In 2006, Shoucheng Zhang predicted that quantum spin Hall effect (QSHE) can be realized in mercury telluride-cadmium telluride semiconductor quantum wells (Bernevig B. A. et al., Quantum spin Hall effect and topological phase transition in HgTe quantum wells, Science, 2006, 314:1757-1761). This prediction was confirmed in 2007 (Konig M. et al. Qauntum spin Hall insulator state in HgTe quantum wells. Science, 2007, 318:766-770). At present, in the variety of quantized forms of the HE, only the quantum anomalous Hall effect (QAHE) has not been observed in reality. QAHE is the QHE in zero magnetic field without Landau levels, which can have a Hall resistance of h/e² (i.e., 25.8 kΩ, i.e., quantum resistance), wherein e is the charge of an electron and h is Planck's constant. The realizing of the QAHE can get rid of the requirement for the external magnetic field and the high electron mobility of the sample, and has an application potential in real devices.

Topological insulators (TIs) are a class of new concept quantum materials. A TI has its bulk band gapped at Fermi level, the same as usual insulators, but hosts gapless, Dirac-type, and spin-split surface states at all of its surfaces, which allow the surfaces to be electrically conductive and are protected by time reversal symmetry (TRS). There are two kinds of TIs, three-dimensional (3D) TIs and two-dimensional (2D) TIs. 3D TIs have topologically-protected two dimensional surface states. 2D TIs have topologically-protected one dimensional edge states. The discovery of Bi₂Se₃ group (including Bi₂Se₃, Bi₂Te₃, and Sb₂Te₃) of TIs makes this kind of material receives substantial research interest from not only condensed matter physics but also material science. In 2010, Yu R. et al. predicted that QAHE could be achieved in Cr or Fe doped Bi₂Se₃, Bi₂Te₃, and Sb₂Te₃ 3D TI films (Yu R. et al., Quantized anomalous Hall effect in magnetic topological insulators, Science, 2010, 329:61-64). However, any TI which can observe the QAHE therein has not been achieved. Further, even a ferromagnetic material (including magnetic doped TIs) having an anomalous Hall resistance larger than a kiloohm (kΩ) has not been achieved. For a film having a thickness of 5 nanometers and having the anomalous Hall resistance larger than a kiloohm, the corresponding anomalous Hall resistivity should be larger than or equal to 0.5 milliohms·millimeter (mΩ·mm).

What is needed, therefore, is to provide a TI structure having a relatively large anomalous Hall resistance.

BRIEF DESCRIPTION OF THE DRAWINGS

Many aspects of the embodiments can be better understood with references to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the embodiments. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.

FIG. 1 is a schematic view of a schematic crystal structure of Sb₂Te₃, wherein (a) is a perspective view, (b) is a top view, and (c) is a side view of 1 QL.

FIG. 2 is a schematic view of an MBE reactor chamber.

FIG. 3 is a scanning tunneling microscope (STM) image of Cr doped Sb₂Te₃.

FIG. 4 is a side view of one embodiment of an electrical device.

FIG. 5 is a top view of one embodiment of the electrical device of FIG. 4.

FIG. 6 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of one embodiment of magnetically doped TI quantum well film at different back gate voltages (V_(b)), wherein a unit of R_(yx) is quantum resistance h/e², which is 25.8 kΩ.

FIG. 7 is a graph showing magnetic field (μ₀H) dependent longitudinal resistances (R_(xx)) of the embodiment of FIG. 6 at different back gate voltages (V_(b)), wherein a unit of R_(xx) is quantum resistance h/e², which is 25.8 kΩ.

FIG. 8 is a graph showing dependences of R_(yx) and R_(xx) on different back gate voltages (V_(b)) of the embodiment of FIG. 6, wherein units of R_(yx) and R_(xx) are both quantum resistance (h/e², i.e., 25.8 kΩ).

FIG. 9 is a graph showing a dependence of arctangent of Hall angle

$\alpha = \frac{R_{yx}}{R_{xx}}$

on different back gate voltages (V_(b)) of the embodiment of FIG. 6.

FIG. 10 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of another embodiment of magnetically doped TI quantum well film at different back gate voltages (V_(b)), wherein the unit of R_(yx) is kΩ.

FIG. 11 is a graph showing magnetic field dependent longitudinal resistances (R_(xx)) of the embodiment of FIG. 10 at different back gate voltages (V_(b)), wherein the unit of R_(xx) is kΩ.

FIG. 12 is a graph showing a dependence of Hall angle

$\alpha = \frac{R_{yx}}{R_{xx}}$

on different back gate voltages (V_(b)) of the embodiment of FIG. 10.

FIG. 13 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of yet another embodiment of magnetically doped TI quantum well film at different back gate voltages (V_(b)), wherein the unit of R_(yx) is quantum resistance (h/e², i.e., 25.8 kΩ).

FIG. 14 is a graph showing magnetic field (μ₀H) dependent longitudinal resistances (R_(xx)) of the embodiment of FIG. 13 at different back gate voltages (V_(b)), wherein the unit of R_(xx) is quantum resistance (h/e², i.e., 25.8 kΩ).

FIG. 15 is a graph showing a dependence of Hall angle

$\alpha = \frac{R_{yx}}{R_{xx}}$

on different back gate voltages (V_(b)) of the embodiment of FIG. 13.

FIG. 16 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of a comparative sample (1) at different back gate voltages (V_(b)), wherein the unit of R_(yx) is Ω.

FIG. 17 is a graph showing a dependence of longitudinal resistance (R_(xx)) on different back gate voltages (V_(b)) of the comparative sample (1) of FIG. 16, wherein the unit of R_(xx) is Ω.

FIG. 18 is a graph showing dependences of R_(yx) and carrier density (n_(2D)) on different back gate voltages (V_(b)) of the comparative sample (1) of FIG. 16, wherein the unit of R_(yx) is Ω.

FIG. 19 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of a comparative sample (2) at different back gate voltages (V_(b)), wherein the unit of R_(yx) is Ω.

FIG. 20 is a graph showing magnetic field (μ₀H) dependent Hall resistances (R_(yx)) of a comparative sample (3) at different back gate voltages (V_(b)), wherein the unit of R_(yx) is Ω.

DETAILED DESCRIPTION

The disclosure is illustrated by way of example and not by way of limitation in the figures of the accompanying drawings in which like references indicate similar elements. It should be noted that references to “an” or “one” embodiment in this disclosure are not necessarily to the same embodiment, and such references mean at least one.

One embodiment of a TI structure is provided. The TI structure includes an insulating substrate and a magnetically doped TI quantum well film located on the insulating substrate. A material of the magnetically doped TI quantum well film is antimony telluride (Sb₂Te₃) doped by chromium (Cr) and bismuth (Bi) substituting some of the Sb in the Sb₂Te₃, which can be represented by a chemical formula Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, wherein 0<x<1, 0<y<2. The doping with Cr introduces hole type charge carriers and the doping with Bi introduces electron type charge carriers into the magnetically doped TI quantum well film. The values of x and y satisfy that the amount of the hole type charge carriers introduced by the doping with Cr is substantially equal to the amount of the electron type charge carriers introduced by the doping with Bi. By satisfying this, the carrier density of the magnetically doped TI quantum well film is equal to or smaller than 1×10¹³ cm⁻² without applying a voltage thereto (i.e., at zero electric field). Thus, the effectiveness of a gate voltage tuning method can be guaranteed during realization of the QAHE by the magnetically doped TI quantum well film. The magnetically doped TI quantum well film has 3 QL to 5 QL, and has a thickness in a range from 3 QL thickness to 5 QL thickness (about 3 nanometers to about 5 nanometers), wherein “QL” means “quintuple layer”. “QL thickness” means the thickness of the quintuple layer.

The magnetically doped TI quantum well film is formed by doping the Sb₂Te₃ with Cr atoms and Bi atoms to replace some of the Sb atoms therein. Sb₂Te₃ is a layer-type material, belonging to the trigonal crystal system, and has a space group of D_(3d) ⁵(R 3m). Referring to FIG. 1, on the xy plane, Sb atoms and Te atoms are respectively arranged in a hexagonal close packing style to form Sb atom layers and Te atom layers. Sb atom layers and Te atom layers are alternately laminated along the direction z perpendicular to the xy plane. Each QL consists of five adjacent atom layers. In Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, the five adjacent atom layers of one QL are the first Te atom layer (Te1), the Cr and Bi doped first Sb atom layer (Sb1), the second Te atom layer (Te2), the Cr and Bi doped second Sb atom layer (Sb1′), and the third Te atom layer (Te1′). In a single QL, the Sb (or Cr, Bi) atoms and Te atoms are joined by covalent-ionic bonds. Between adjacent QLs, the Te1 and Te1′ are combined by van der Waals force, thus forming cleavage planes between adjacent QLs. In Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, the values of x and y satisfy that the amount of the hole type charge carriers introduced by the doping with Cr is substantially equal to the amount of the electron type charge carriers introduced by the doping with Bi. In one embodiment, 0.05<x<0.3, 0<y<0.3, and 1:2<x:y<2:1 (e.g., 2:3≦x:y≦25:22).

The material of the insulating substrate is not limited, and only needs to be capable of having the magnetically doped TI quantum well film located, grown, and/or formed thereon by a molecular beam epitaxy (MBE) method. In one embodiment, the material of the insulating substrate can have a dielectric constant greater than 5000 at a temperature equal to or smaller than 10 Kelvin (K), such as strontium titanate (STO). To achieve a large anomalous Hall resistance, or even achieve the QAHE, a chemical potential of the magnetically doped TI quantum well film is tuned by applying an external electric field or voltage to the magnetically doped TI quantum well film which is called the gate voltage tuning method. More specifically, the electric field or voltage can be applied to the magnetically doped TI quantum well film through a top gate and/or a back gate on the TI structure. The chemical potential of the magnetically doped TI quantum well film can be tuned by the field effect. To achieve the large anomalous Hall resistance, or even achieve the QAHE, the defects in the magnetically doped TI quantum well film need to be as few as possible to decrease the carrier density in the magnetically doped TI quantum well film. However, the top gate is formed by forming a dielectric layer and a metal electrode on a surface of the magnetically doped TI quantum well film, which increases the possibility of destroying the magnetically doped TI quantum well film or introducing defects into the magnetically doped TI quantum well film. The insulating substrate, having a relatively large dielectric constant at a relatively low temperature, can have a relatively large capacitance, though the thickness of the insulating substrate is relatively large. Thus, the insulating substrate having the relatively large dielectric constant can be directly used as the dielectric layer at the relatively low temperature between the back gate and the magnetically doped TI quantum well film. The insulating substrate has a first surface and a second surface, that is opposite to the first surface. The magnetically doped TI quantum well film can be formed on the first surface. The back gate is formed by forming a metal electrode on the second surface of the insulating substrate. The forming of the back gate does not contact to the magnetically doped TI quantum well film, thus avoids of introducing defects to the magnetically doped TI quantum well film. When the material of the insulating substrate is STO, the magnetically doped TI quantum well film can be grown on a (111) surface, which is used as the first surface. The (111) surface is a surface along a (111) crystallographic plane of the STO. The thickness of the STO insulating substrate can be in a range from about 0.1 millimeters to about 1 millimeter.

The magnetically doped TI quantum well film can be formed on the insulating substrate through a molecular beam epitaxy (MBE) method. One embodiment of a method for forming the TI structure having the STO substrate includes following steps of:

S11, providing the STO substrate having the (111) surface, the STO substrate is disposed in a ultra-high vacuum environment in an MEB reactor chamber;

S12, cleaning the surface of the STO substrate by heat-treating the STO substrate in the MEB chamber;

S13, heating the STO substrate and forming Bi beam, Sb beam, Cr beam, and Te beam in the MEB chamber in a controlled ratio achieved by controlling flow rates of the Bi beam, Sb beam, Cr beam, and Te beam; and

S14, forming the magnetically doped TI quantum well film on the (111) surface of the STO substrate, wherein the controlled ratio of the Bi beam, Sb beam, Cr beam, and Te beam makes that in the magnetically doped TI quantum well film, the amount of the hole type charge carriers introduced by the doping with Cr is substantially equal to the amount of the electron type charge carriers introduced by the doping with Bi.

In the step S11, the (111) surface of the STO substrate is smooth at atomic level. In one embodiment, the (111) surface of the STO substrate is formed by steps of: cutting the STO substrate along the (111) crystallographic plane; heating the STO substrate in deionized water below 100° C. (e.g., 70° C.); and burning the STO substrate in an environment of a combination of O₂ and Ar at a temperature in a range from about 800° C. to about 1200° C. (e.g., 1000° C.). A time period for the heating in the deionized water can be in a range from about 1 hour to about 2 hours. A time period for the burning in the environment of the combination of O₂ and Ar can be in a range from about 2 hours to about 3 hours.

MEB is a film evaporation-deposition method performed in ultra-high vacuum (in a range from 1.0×10⁻¹¹ mbar to 1.0×10⁻⁹ mbar, e.g., about 1.0×10⁻¹⁰ mbar) at a deposition rate in a range from about 0.1 nm/s to about 1 nm/s to evaporate a source and deposite the film at a low speed which allows films to grow epitaxially. The absence of carry gases as well as the ultra high vacuum environment results in the highest achievable purity of grown films. The MBE reactor chamber can be joined with a variable temperature scanning tunneling microscope (VTSTM) and angle resolved photoemission spectroscopy (ARPES) to form a system. The system can have in-situ VTSTM and ARPES tests of the magnetically doped TI quantum well film.

During the forming of the magnetically doped TI quantum well film and the VTSTM and ARPES tests of the magnetically doped TI quantum well film, the magnetically doped TI quantum well film is kept in the MBE reactor chamber having a degree of vacuum smaller than 1.0×10⁻¹⁰ mbar (a pressure is less than 1.0×10⁻⁸ Pa). In this degree of vacuum, the density of the gas molecules at room temperature is about 2.4×10⁶/cm³, and the average distance between the gas molecules is about 0.1 millimeters. In this ultra-high vacuum environment, the magnetically doped TI quantum well film having high purity and few defects can be formed using the MBE method. Meanwhile, in this ultra-high vacuum environment, the (111) surface of the magnetically doped TI quantum well film can be kept clean for a long time. In one embodiment, the MBE reactor chamber has a degree of vacuum less than or equal to 5.0×10⁻¹° mbar.

In the step S12, the temperature and time of the heat-treating are selected to make the (111) surface of the STO substrate as clean as possible. In one embodiment, the temperature of the heat-treating is about 600° C., and the time of the heat-treating is about 1 hour to about 2 hours. The heat-treating can remove organic substances, gas, and water adsorbed on the (111) surface of the STO substrate.

In the step S13, the beams of Bi, Sb, Cr, and Te can be generated by heating evaporating sources of Bi, Sb, Cr and Te. FIG. 2 shows that in the reactor chamber, four independent evaporating sources can be arranged by respectively disposing solid Bi, Sb, Cr, and Te in four Knudsen cells (K-Cell). One Knudsen cell is composed of a crucible, a heating filament, a water cooling system, an orifice shutter, and a thermocouple. A material of the crucible can be pyrolytic boron nitride or Al₂O₃. The solid Bi, Sb, Cr, and Te are respectively disposed in the crucibles. All the solid Bi, Sb, Cr, and Te have the purity larger than or equal to 5N degree (99.999%). The heating filaments (e.g., tantalum filaments or tungsten filaments) are used to heat the crucibles to evaporate the solid Bi, Sb, Cr, and Te, and the evaporating rate is controlled by controlling the heating temperature. The orifice shutter is used to cover the crucible to control the beginning and ending of the evaporation. Thus, the uniformity of the ratio among the Bi, Sb, Cr, and Te in the formed magnetically doped TI quantum well film can be controlled. The water cooling system is used to decrease the temperature around the evaporating source, thus keeps a relatively good vacuum and decreases the impurity in the MBE reactor chamber. The STO substrate is disposed in the MEB reactor chamber and spaced from the evaporating sources. The (111) surface of the STO substrate faces to the evaporating sources. A heater can be further located on a back side (e.g., near the second surface) of the STO substrate opposite to the (111) surface to heat the STO substrate.

The flow rate can be a mass flow rate or a volumetric flow rate, which is a mass or a volume of a fluid passing through a given surface per unit of time. The flow rates of Bi, Sb, Cr, and Te are represented as V_(Bi), V_(Sb), V_(Cr), and V_(Te) respectively, and satisfy V_(Te)>(V_(Cr)+V_(Bi)+V_(Sb)), to ensure that the magnetically doped TI quantum well film is formed in a Te environment, to decrease the amount of Te vacancies in the magnetically doped TI quantum well film. In one embodiment, (V_(Cr)+V_(Bi)+V_(Sb)):V_(Te) is in a range from about 1:10 to about 1:15. However, the V_(Te) cannot be too large. A relatively large V_(Te) tends to induce an aggregation of the Te atoms on the (111) surface of the STO substrate. The V_(Bi), V_(Sb), V_(Cr), and V_(Te) can be controlled by controlling the temperatures of the four evaporating sources, and can be measured by a flow meter (e.g., quartz oscillation type gas flow meter).

In step S14, during the forming of the magnetically doped TI quantum well film, the STO substrate may need to be heated to a proper temperature (e.g., in a range from about 180° C. to about 250° C.). The temperature of the heating of the STO substrate can ensure the decomposition of Te_(e) and/or Te_(o) molecule into Te atoms, while ensuring the formation of a single crystal magnetically doped TI quantum well film. An approximate value of the ratio among the Bi, Sb, Cr, and Te in the magnetically doped TI quantum well film can be estimated by the flow meter, and an accurate value can be achieved by chemical element analysis of a thick sample (e.g., having a thickness of 100 QL) formed by the same method. In one embodiment, the heating temperature of the substrate (T_(sub)) is about 180° C. to about 200° C., the evaporating temperature of Te source (T_(Te)) is about 310° C., the evaporating temperature of Bi source (T_(Bi)) is about 500° C., the evaporating temperature of Sb source (T_(Sb)) is about 360° C., and the evaporating temperature of Cr source (T_(Cr)) is about 1020° C. The STO substrate can be heated by tungsten filaments disposed on the back side of the STO substrate. In one embodiment, when the magnetically doped TI quantum well film is a 5 QL film, the first QL of the magnetically doped TI quantum well film is formed at a lower heating temperature of the STO substrate (e.g., T_(sub)=180° C.), and the other 4 QL are formed on the first QL at a higher heating temperature (e.g., T_(sub)=200° C.). A high temperature of the STO substrate may cause the surface of the first QL to be uneven. These two temperature periods can ensure that the first QL uniformly and flat on the substrate at a lower temperature, and the other 4 QL can have a high quality at the higher temperature.

After step S14, a step of annealing the magnetically doped TI quantum well film can be processed to further decrease the defects in the magnetically doped TI quantum well film. The magnetically doped TI quantum well film can be heated at an annealing temperature for an annealing time. In one embodiment, the annealing temperature can be in a range from about 180° C. to about 250° C. (e.g., 200° C.), an annealing time can be in a range from about 10 minutes to about 1 hour (e.g., 20 minutes).

Formation of the TI structure is not limited to the above described method. In another embodiment, the material of the insulating substrate can be Al₂O₃, and the insulating substrate can be a single crystal sapphire substrate. However, because the dielectric constant of sapphire is only about 20 at a low temperature, the sapphire substrate cannot be used as the dielectric layer for the back gate. Thus, the top gate structure may be used to tune the chemical potential of the magnetically doped TI quantum well film. More specifically, a solid dielectric layer (e.g., Al₂O₃ film, HfO₂ film, or MgO film) having a small thickness (e.g., 300 nanometers) can be formed on the surface of the magnetically doped TI quantum well film, and a metal electrode as the top gate can then be formed on the surface of the dielectric layer.

In another embodiment, to avoid damaging or negatively affecting the structure of the magnetically doped TI quantum well film, a liquid top gate structure can be used to tune the chemical potential. More specifically, a liquid dielectric layer can be formed by dropping a drop of ionic liquid on the surface of the magnetically doped TI quantum well film, and a metal electrode as the top gate can be arranged to be in contact with the liquid dielectric layer but spaced from the magnetically doped TI quantum well film.

As mentioned in the background, Sb₂Te₃ TI film makes it possible to realize the QAHE. Theoretically, Cr can equivalently substitute Sb of the Sb₂Te₃ to achieve the Cr doped Sb₂Te₃. The QAHE can be achieved by doping the Sb₂Te₃ TI film with Cr having an infinite uniformity to achieve the ferromagnetism of the TI film. This ferromagnetism achieved by the doping is different from RKKY type ferromagnetism in traditional diluted magnetic semiconductors and does not need charge carriers, thus keeping the system in the insulating state.

However, the inventors found that in a real system, the carrier density in the Cr doped Sb₂Te₃ is very large. The carrier density can be calculated by n_(2D)=1/eR_(H), wherein R_(H) is a slope (or gradient) of a Hall curve (i.e., a curve of magnetic field to Hall resistance). The tested carrier density of the Sb₂Te₃ quantum well film with Cr doped on Sb sites has a carrier density in a scale of 10¹⁴ cm⁻². It is impossible to tune that large of a carrier density by using either back gate structure or top gate structure. That large of a carrier density is mainly caused by the defects introduced during the Cr doping of the Sb₂Te₃. Numerous factors such as forming conditions and environment conditions affect the forming of the film. It is extremely difficult to dope the Sb₂Te₃ with Cr to the infinite degree of uniformity. During the Cr doping, the defects are introduced into the Sb₂Te₃ quantum well film. FIG. 3 shows that an image of Cr doped Sb₂Te₃ at atomic resolution achieved by VTSTM, the triangle shaped defects are the locations of Cr dopants. Theoretically, the substitution of Sb atoms with Cr atoms does not introduce extra charge carriers. However, in a real system, the doping cannot be infinitely uniform. Non-bonded Cr atoms can exist in the film and introduce extra charge carriers, which is the hole type charge carriers tested by inventors. The carrier density is too large to be decreased to a level to realize the QAHE.

In the present disclosure, Sb₂Te₃ is doped by both Cr and Bi to form a quaternary system in the film. The doping of Sb₂Te₃ with Cr and Bi can simultaneously introduce two adverse types of defects. The defects (hole type) introduced by Cr can be substantially neutralized by the defects (electron type) introduced by another kind of dopant (e.g., Bi), thus decreasing the carrier density in the material. Thus, the quaternary system can have the ferromagnetic property while having a low level of carrier density. The amount of Bi doped in the Sb₂Te₃ (i.e., the value of x in Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃) depends on the amount of defects introduced by Cr. The amount of defects introduced by Cr may be affected by factors such as forming conditions and environmental conditions. The amount of defects introduced by Cr can be analyzed previously by forming a Cr_(y)Sb_(2-y)Te₃ film under the same conditions. In one embodiment, 0.05<x<0.3, 0<y<0.2, and 1:2<x:y<2:1 (e.g., 2:3≦x:y≦25:22). By adjusting the amount of Bi and Cr (i.e., adjusting the values of x and y), the amount of the hole type charge carriers introduced by the doping with Cr is substantially equal to the amount of the electron type charge carriers introduced by the doping with Bi, and the carrier density in the magnetically doped TI quantum well film can be decreased to a level that is capable of being tuned by the gate tuning method. By using the gate tuning method to tune the quaternary system, the magnetically doped TI quantum well film can have the carrier density near zero, and have the anomalous Hall resistance (R_(AH)) in a range of 0.3×25.8 kΩ≦R_(AH)≦1×25.8 kΩ (i.e., 7.74 kΩ≦R_(AH)≦25.8 kΩ), while the anomalous Hall angle is (α=R_(AH)/R_(xx))≧0.2.

An embodiment of an electrical device based on the TI structure is provided. The electrical device includes the above described TI structure. The TI structure includes an insulating substrate including a first surface and a second surface opposite to the first surface, and a magnetically doped TI quantum well film grown on the first surface of the insulating substrate. A material of the magnetically doped TI quantum well film is represented by a chemical formula of Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, wherein 0<x<1, 0<y<2. The doping with Cr introduces hole type charge carriers and the doping with Bi introduces electron type charge carriers into the magnetically doped TI quantum well film. The values of x and y satisfy that the amount of the hole type charge carriers introduced by the doping with Cr is substantially equal to the amount of the electron type charge carriers introduced by the doping with Bi. The magnetically doped TI quantum well film is in a range from 3 QL thickness to 5 QL thickness.

In one embodiment, the electrical device further includes a back gate electrode and two conducting electrodes (i.e., source electrode and drain electrode). The back gate electrode is used to tune the chemical potential of the magnetically doped TI quantum well film. The two conducting electrodes are used to conduct an electrical current through the magnetically doped TI quantum well film along a first direction.

In one embodiment, the electrical device can further include three output electrodes (e.g., E1, E2 and E3), which are used to test the resistances of the magnetically doped TI quantum well film in the first direction (i.e., the longitudinal resistance) and in the second direction (i.e., the Hall resistance).

All the above mentioned electrodes can be formed by using an E-beam method. The material of the electrodes can be selected according to having good conductivity (e.g., gold or titanium). In another embodiment, the electrodes can be formed by coating an indium paste or silver paste on the surface of the TI structure.

More specifically, the back gate electrode is located on the second surface of the insulating substrate. The two conducting electrodes and three output electrodes are arranged on the top surface of the magnetically doped TI quantum well film and spaced from each other. The two conducting electrodes and three output electrodes are electrically connected to the magnetically doped TI quantum well film. The two conducting electrodes are arranged at two opposite sides of the magnetically doped TI quantum well film. A line extending from one conducting electrode to the other conducting electrode is the first direction. A line extending from E1 to E2 is the first direction, and a line extending from E2 to E3 is the second direction. The first direction is perpendicular to the second direction. The E1, E2 and E3 can be arranged at two opposite sides in the second direction of the magnetically doped TI quantum well film. For example, E1 and E2 can be arranged to the same side, and E3 can be arranged on the other side. The two conducting electrodes can be bar shaped with a relatively long length approximately equal to the length of the magnetically doped TI quantum well film in the second direction. The length direction of the conducting electrodes can be parallel to the second direction. The three output electrodes can be spot electrodes.

Referring to FIG. 4 and FIG. 5, in the figure, x represents the first direction and y represents the second direction. In one embodiment of the electrical device 10, the magnetically doped TI quantum well film 20 formed on the first surface of the insulating substrate 30 has a shape including a rectangular central part 22, two first connecting parts 24 extended from the central part 22 to the two conducting electrodes 50, and three second connecting parts 26 extended from the central part 22 to the E1, E2, and E3. The three second connecting parts 26 are spaced from each other. The length of the central part 22 in the second direction is smaller than the length of the conducting electrode 50. The first connecting parts 24 can have a trapezoid shape having two parallel sides parallel to the second direction, the longer one is joined to the conducting electrode 50, the shorter one is joined to the central part 22. The three second connecting parts 26 can extend along the second direction. In one embodiment, the three second connecting parts 26 can extend from three corners of the rectangle central part 22 to E1, E2, and E3. The back gate electrode 40 is located on the second surface of the insulating substrate 30.

The conducting electrode 50 can be located on a top surface of the first connecting parts 24 at a side. The pattern of the magnetically doped TI quantum well film 20 having the narrow rectangular central part 22 and the trapezoid shaped first connecting parts 24 connected to the long conducting electrode 50 can decrease the contacting resistance. The second connecting part 26 can have a strip shape with a narrow width. The output electrode is located on a top surface of the second connecting part 26 at one end. The other end of the second connecting part 26 is joined to the central part 22.

The rectangular central part 22 can have a length of about 100 microns to about 400 microns (e.g., 200 microns) in the first direction, and a length of about 10 microns to about 40 microns (e.g., 20 microns) in the second direction.

The conducting electrode 50 can have a length of about 1 millimeter to about 4 millimeters (e.g., 2 millimeters) in the second direction, and a length of about 5 millimeters to about 10 millimeters in the first direction.

In addition, the electrical device can further include a fourth output electrode E4 similar to E1, E2, and E3. E4 is spaced from E1, E2, and E3, and located on a surface of the magnetically doped TI quantum well film 20. A direction from E3 to E4 is the first direction, and a direction from the E1 to E4 is the second direction. Correspondingly, the magnetically doped TI quantum well film 20 can includes four second connecting parts 26 respectively extended from the central part 22 to E1, E2, E3, and E4 from the four corners of the central part 22.

The pattern of the magnetically doped TI quantum well film 20 can formed by removing other portion of the magnetically doped TI quantum well film 20 by mechanical scraping method, ultraviolet lithography method, or electron beam lithography method.

An embodiment of a method for generating QAHE includes steps of:

-   -   S21, forming a TI quantum well film in a 3 QL thickness to 5 QL         thickness on the insulating substrate;     -   S22, doping the TI quantum well film with a first chemical         element and a second chemical element during the forming of the         TI quantum well film to form the magnetically doped TI quantum         well film, the doping with the first chemical element and the         second chemical element respectively introducing hole type         charge carriers and electron type charge carriers in the         magnetically doped TI quantum well film, to decrease the carrier         density of the magnetically doped TI quantum well film to be         smaller than or equal to 1×10¹³ cm⁻², one of the first element         and the second element magnetically doping the TI quantum well         film (i.e., one of the first element and the second element is         the magnetically dopant to the topological insulator quantum         well film);     -   S23, applying an electric field to the magnetically doped TI         quantum well film to further decrease the carrier density at         which the QAHE is achieved.

In step S23, when the insulating substrate has a relatively large dielectric constant, the electric field can be applied only by the back gate structure. The electric field can be in a range of ±200V. Step S23 can be processed at a low temperature (e.g., smaller than or equal to 10 Kelvin (K)). In one embodiment, the step S23 is processed at a temperature smaller than or equal to 1.5 K.

The method for generating QAHE can solve the problem that the magnetically doping of the TI quantum well film (e.g., Cr doping) may introduce defects by introducing an adverse type of defects by another dopant and applying the electric field, thus effectively decreases the carrier density to a extremely low level (e.g., below 1×10¹² cm⁻²) to realize QAHE.

Experiments on Some Embodiments

Different embodiments of the electrical devices are formed by using different magnetically doped TI quantum well films. During an experiment of an electrical device, constant electric current is conducted through the magnetically doped TI quantum well film by the two conducting electrodes at a low temperature. Resistances R_(xx) and R_(yx) in different directions of the magnetically doped TI quantum well film are measured by using the three output electrodes, wherein R_(xx) is the resistance along the direction of the constant electric current (i.e., the first direction), and R_(yx) is the resistance along the direction perpendicular to the constant electric current (i.e., the second direction). The R_(yx) is the Hall resistance. Top gate structure or back gate structure may be used to tune the chemical potential of the magnetically doped TI quantum well film in the experiment. The top gate voltage is represented by V_(t), and the back gate voltage is represented by V_(b). The magnetic property of the magnetically doped TI quantum well film is studied by a superconducting quantum interference device (SQUID).

In the magnetic materials, R_(yx)=R_(A)M(T,H)+R_(N)H, wherein R_(A) is the anomalous Hall coefficient, M(T,H) is the magnetization, R_(N) is the normal Hall coefficient. H is an external magnetic field. The value of the anomalous Hall resistance is defined as the value of the Hall resistance (R_(yx)) at zero magnetic field. The R_(A)M(T,H) is the anomalous Hall resistance (R_(AH)=R_(A)M(T,H)), which is related to the magnetization (i.e., M(T,H)), and plays the major part of R_(yx) at a low magnetic field. The R_(N)H is the normal Hall resistance, which is the linear part of R_(yx) at a high magnetic field. R_(N) decides the carrier density (n_(2D)), and the type of the charge carriers. The following experiments are processed at near zero magnetic field (i.e., H=0). Thus, the R_(yx) can be seen as equal to the R_(AH).

Embodiment 1 T=30 mK, 5 QL Sample, Back Gate Structure

The magnetically doped TI quantum well film is 5 QL Cr_(0.15)(Bi_(0.10)Sb_(0.9))_(1.85)Te₃ (i.e., the film has 5 QL), and the substrate 30 is STO substrate, in the embodiment 1. Different back gate voltages (Vb) are applied to the magnetically doped TI quantum well film, and the corresponded Hall curves are tested at the temperature of 30 mK.

Referring to FIGS. 6 to 9, H is the magnetization and μ₀ is the vacuum permeability, in the μ₀H. The unit of μ₀H is Tesla (T). The R_(AH) of the sample is changed with V_(b), and the hysteresis phenomena can be seen, which means that the sample has a good ferromagnetic property. When 0V≦V_(b)≦10V, the change of R_(AH) with V_(b) is not very great. When V_(b)=−4.5 V, R_(AH)=25.8 kΩ.

Embodiment 2 T=1.5K, 4 QL Sample, Back Gate Structure

The magnetically doped TI quantum well film is 4 QL Cr_(0.22)(Bi_(0.22)Sb_(0.78))_(1.78)Te₃, and the substrate 30 is STO substrate, in the embodiment 2.

Different back gate voltages (V_(b)) are applied to the magnetically doped TI quantum well film, and the corresponded Hall curves are tested at the temperature of 1.5K. Referring to FIG. 10, the hysteresis phenomena can be seen, and the hysteresis loops have a “square” shape, which means that the sample has a great ferromagnetic property. By changing V_(b), a relatively large R_(AH) can be achieved. The R_(AH) increases first and then decreases with the increasing of the V_(b). When V_(b)=45 V, R_(AH) reaches the maximum value, which is 10 kΩ. This value is approximate to 0.4 quantum resistance, the quantum resistance is 25.8 kΩFIG. 11 shows that the R_(xx)-μ₀H curves show a butterfly shaped hysteresis pattern, which also reveals that the sample has a great ferromagnetic property. In addition, when V_(b)=45V, the anomalous Hall angle (α=R_(AH)/R_(xx)) is as high as 0.42, which is twice of that value of the 5 QL sample. FIG. 12 shows that the Hall angle (R_(yx)/R_(xx)) increases first and then decreases with the increasing of the V_(b).

Embodiment 3 T=100 mK, 4 QL Sample, Back Gate Structure

The magnetically doped TI quantum well film is 4 QL

Cr_(0.22)(Bi_(0.22)Sb_(0.78))_(1.78)Te₃, and the substrate 30 is STO substrate, in the embodiment 3.

Different back gate voltages (V_(b)) are applied to the magnetically doped TI quantum well film, and the corresponded Hall curves are tested at the temperature of 100 mK. FIG. 13 shows that the hysteresis phenomena can be seen, which means that the sample has a good ferromagnetic property. When 0V≦V_(b)≦20V, the change of R_(AH) with V_(b) is not very great. R_(AH) is about 0.6 quantum resistance. When V_(b)=10 V, R_(AH) reaches the maximum value, (R_(AH))_(max)=0.59 h·e⁻², which is about 15.3 kΩ. This value exceeds a half of quantum resistance and is larger than the greatest known anomalous Hall resistance ever achieved in the world at this time. FIG. 14 shows that the change of the R_(xx) with the change of the V_(b) is more obviously than the change of the R_(yx) with the change of V_(b) as shown in FIG. 13. Especially, when V_(b)=0V, the anomalous Hall angle (α=R_(AH)/R_(xx))>0.5. FIG. 15 shows that the Hall angle (R_(yx)/R_(xx)) increases first and then decreases with the increasing of the V_(b).

Embodiment 4 T=90 mK, 5 QL Sample, Back Gate Structure, V_(t)=0

The magnetically doped TI quantum well film is 5 QL Cr_(0.15)(Bi_(0.1)Sb_(0.9))_(1.85)Te₃, and the substrate 30 is STO substrate having a thickness of 0.25 millimeters, in the embodiment 4. Different back gate voltages (V_(b)) are applied to the magnetically doped TI quantum well film at the temperature of 90 mK. When V_(b)=30 V, the maximum R_(AH) is about 24.1 kΩ.

Embodiment 5 T=400 mK, 5 QL Sample, Back Gate Structure, V_(t)=0

The magnetically doped TI quantum well film is 5 QL Cr_(0.15)(Bi_(0.1)Sb_(0.9))_(1.85)Te₃, and the substrate 30 is STO substrate having a thickness of 0.25 millimeters, in the embodiment 5. Different back gate voltages (V_(b)) are applied to the magnetically doped TI quantum well film at the temperature of 400 mK. When V_(b)=20 V, the maximum R_(AH) is about 23.0 kΩ.

Embodiment 6 T=1.5 K, 5 QL Sample, Back Gate Structure, V_(t)=0

The magnetically doped TI quantum well film is 5 QL Cr_(0.15)(Bi_(0.1)Sb_(0.9))_(1.85)Te₃, and the substrate 30 is STO substrate having a thickness of 0.25 millimeters, in the embodiment 6. Different back gate voltages (V_(b)) are applied to the magnetically doped TI quantum well film at the temperature of 1.5 K. When V_(b)=28 V, the maximum R_(AH) is about 19.02 kΩ.

The experiment results of the embodiments 1 to 6 are shown in the Table 1.

TABLE 1 Hall V_(b) R_(AH) resistivity, ρ_(yx) R_(xx) No. Sample Thickness Temperature (V) (kΩ) (μΩ · m) (kΩ) R_(AH)/R_(xx) 1 Cr_(0.15)(Bi_(0.10)Sb_(0.9))_(1.85)Te₃ 5QL  30 mK −4.5 25.8 127.3 3.4 7.58 2 Cr_(0.22)(Bi_(0.22)Sh_(0.78))_(1.78)Te₃ 4QL 1.5K 45 10 50 23.8 0.42 3 Cr_(0.22)(Bi_(0.22)Sh_(0.78))_(1.78)Te₃ 4QL 100 mK 10 15.3 76.5 34 0.45 4 Cr_(0.15)(Bi_(0.1)Sb_(0.9))_(1.85)Te₃ 5QL  90 mK 30 24.1k 120 7 3.44 5 Cr_(0.15)(Bi_(0.10)Sb_(0.9))_(1.85)Te₃ 5QL 400 mK 20 23.0 115 13 1.7 6 Cr_(0.15)(Bi_(0.10)Sb_(0.9))_(1.85)Te₃ SQL 1.5K 28 19.02 95.1 18.88 1.0007

Comparative Examples

(1) Sb_(2-y)Cr_(y)Te₃

By changing the doping amount of Cr, the material of Cr doped Sb₂Te₃ TI quantum well film can be represented as Sb_(2-y)Cr_(y)Te₃. Four samples of 5 QL Sb_(2-y)Cr_(y)Te₃ TI quantum well films are formed on the (111) surface of the STO substrate, wherein y is 0, 0.05, 0.09, and 0.14 respectively. The experiment results reveal that when y=0, Sb_(2-y)Cr_(y)Te₃ is Sb₂Te₃, and 5 QL Sb₂Te₃ has a linear dispersion surface state, the Dirac point is located above the Fermi level (E_(F)) and at 65 meV. When doping Cr to the Sb₂Te₃, the location of the Dirac point moves from +75 meV when y=0.05 to +88 meV when y=0.14. The E_(F) of all the four samples is not at a magnetically induced gap-opening.

Without Bi doping, the 5 SQL Sb_(1.91)Cr_(0.09)Te₃ TI quantum well films are tuned by using the back gate structure. FIG. 16 and FIG. 17 show that R_(xx) always increases with the increasing of V_(b), which is a typical hole type semiconductor behavior. Thus, it can be known that the tuning has no affection to the type of carriers. The carrier type does not change during the tuning step. During the tuning step, the mobility (μ) does not change, and bases on the equation R_(xx) ⁻¹xx=σ_(xx)=μn_(2D)e, it shows that n_(2D) decreases with the increasing of V_(b) in FIG. 18. FIG. 16 is the Hall curves of the 5 QL Sb_(1.91)Cr_(0.09)Te₃ at different V_(b) when T=1.5 K. The voltage range of the V_(b) is from about −210 V to about +210 V. The anomalous Hall resistance (R_(AH)) always increases with the increasing of V_(b).

When V_(b)=−210 V, R_(AH)=24.152, and n_(2D)=3.4×10¹⁴ cm⁻². When V_(b)=+210V, R_(AH)=40.8, and n_(2D)=9.7×10¹³ cm⁻². The relations between R_(AH) and n_(2D) to V_(b) are shown in FIG. 18. It can be seen from the FIG. 18 that R_(AH) increases with the decreasing of n_(2D). This phenomenon is completely different from the traditional diluted magnetic semiconductors. In the diluted magnetic semiconductor, the larger the n_(2D), the larger the R_(AH). However, the R_(AH) is still to low to achieve QAHE.

(2) Bi_(1.78)Cr_(0.22)Se₃

By changing the doping amount of Cr, the material of Cr doped Bi₂Se₃ TI quantum well film can be represented as Bi_(2-y)Cr_(y)Se₃. By selecting y=0.22, the thickness is 10 QL thickness, a sample of 10 QL Bi_(1.78)Cr_(0.22)Se₃ TI quantum well film is formed. Referring to FIG. 19, when T=1.5K, there is no hysteresis loop observed in the Hall effect experiment, which indicates that Cr doped Bi₂Se₃ is a paramagnetic material. Therefore, the Cr doped Bi₂Se₃ cannot have the QAHE.

(3) Bi_(1.78)Cr_(0.22)Te₃

By changing the doping amount of Cr, the material of Cr doped Bi₂Te₃ TI quantum well film can be represented as Bi_(2-y)Cr_(y)Te₃. By selecting y=0.22, the thickness is 10 QL thickness, a sample of 10 QL Bi_(1.78)Cr_(0.22)Te₃ TI quantum well film is formed. FIG. 20 shows that when T=25K, there is hysteresis loops observed in the Hall effect experiment, which indicates that Cr doped Bi₂Se₃ is a ferromagnetism material.

It is to be understood that the above-described embodiment is intended to illustrate rather than limit the disclosure. Variations may be made to the embodiment without departing from the spirit of the disclosure as claimed. The above-described embodiments are intended to illustrate the scope of the disclosure and not restricted to the scope of the disclosure.

It is also to be understood that the above description and the claims drawn to a method may include some indication in reference to certain steps. However, the indication used is only to be viewed for identification purposes and not as a suggestion as to an order for the steps. 

What is claimed is:
 1. A topological insulator structure, comprising: an insulating substrate; and a magnetically doped topological insulator quantum well film located on the insulating substrate; wherein a material of the magnetically doped topological insulator quantum well film is represented by a chemical formula of Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, wherein 0<x<1, 0<y<2, and values of x and y satisfies that an amount of a hole type charge carriers introduced by a doping with Cr is substantially equal to an amount of an electron type charge carriers introduced by a doping with Bi; and the magnetically doped topological insulator quantum well film is in a range of 3 QL thickness to 5 QL thickness.
 2. The topological insulator structure of claim 1, wherein 0.05<x<0.3, 0<y<0.3, and 1:2<x:y<2:1.
 3. The topological insulator structure of claim 2, wherein 2:3≦x:y≦25:22.
 4. The topological insulator structure of claim 1, wherein the magnetically doped topological insulator quantum well film is in 5 QL thickness.
 5. The topological insulator structure of claim 1, wherein a material of the insulating substrate comprises strontium titanate.
 6. The topological insulator structure of claim 1, wherein the magnetically doped topological insulator quantum well film is 5 QL Cr_(0.15)(Bi_(0.10)Sb_(0.9))_(1.85)Te₃, and the material of the insulating substrate is strontium titanate.
 7. The topological insulator structure of claim 1, wherein a carrier density of the magnetically doped topological insulator quantum well film is below 1×10¹³ cm⁻².
 8. The topological insulator structure of claim 1, wherein an anomalous Hall resistance of the magnetically doped topological insulator quantum well film is represented by R_(AH), and 7.74 kΩ≦R_(AH)≦25.8 kΩ, an anomalous Hall angle is represented by α, and α≧0.2.
 9. A topological insulator structure, comprising: an insulating substrate; and a magnetically doped topological insulator quantum well film located on the insulating substrate; wherein a material of the magnetically doped topological insulator quantum well film is represented by a chemical formula of Cr_(y)(Bi_(x)Sb_(1-x))_(2-y)Te₃, wherein 0<x<1, 0<y<2, the magnetically doped topological insulator quantum well film is in a range of 3 QL thickness to 5 QL thickness, and satisfies 7.74 kΩ≦R_(AH)≦25.8 kΩ, and α≧0.2, wherein R_(AH) represents an anomalous Hall resistance and α represents an anomalous Hall angle of the magnetically doped topological insulator quantum well film.
 10. The topological insulator structure of claim 1, wherein a carrier density of the magnetically doped topological insulator quantum well film is below 1×10¹³ cm⁻². 